Will Bergman and Mike Ma

Slides:



Advertisements
Similar presentations
Simple Harmonic Motion and Waves December 1, 2010
Advertisements

 Modeling Harmonic Oscillations and its Applications By Dallas Gosselin and Jonathan Fernandez.
Lesson 1 - Oscillations Harmonic Motion Circular Motion
FCI. Prof. Nabila.M.Hassan Faculty of Computer and Information Basic Science department 2013/ FCI.
Chapter 14 Oscillations
Simple Harmonic Motion. Analytical solution: Equation of motion (EoM) Force on the pendulum constants determined by initial conditions. The period of.
Physics 151: Lecture 30, Pg 1 Physics 151: Lecture 33 Today’s Agenda l Topics çPotential energy and SHM çResonance.
A spring with a mass of 6 kg has damping constant 33 and spring constant 234. Find the damping constant that would produce critical damping
Ch 15 Oscillatory Motion 15-1 Motion of an Object Attached to a Spring Acos  F s = -kx.
College and Engineering Physics Quiz 9: Simple Harmonic Motion 1 Simple Harmonic Motion.
The Simple Pendulum An application of Simple Harmonic Motion
© 2007 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching their.
Passive Acoustic Radiators Justin Yates, Wittenberg University Spring 2014.
Solving the Harmonic Oscillator
13. Oscillatory Motion. Oscillatory Motion 3 If one displaces a system from a position of stable equilibrium the system will move back and forth, that.
Motion of a mass at the end of a spring Differential equation for simple harmonic oscillation Amplitude, period, frequency and angular frequency Energetics.
Lecture 22 Second order system natural response Review Mathematical form of solutions Qualitative interpretation Second order system step response Related.
Damped Oscillations (Serway ) Physics 1D03 - Lecture 35.
Energy of the Simple Harmonic Oscillator. The Total Mechanical Energy (PE + KE) Is Constant KINETIC ENERGY: KE = ½ mv 2 Remember v = -ωAsin(ωt+ ϕ ) KE.
Chapter 14 Periodic Motion. Hooke’s Law Potential Energy in a Spring See also section 7.3.
Welastic = 1/2 kx02 - 1/2 kxf2 or Initial elastic potential energy minus Final elastic potential energy.
Lecture 2 Differential equations
Oscillators fall CM lecture, week 4, 24.Oct.2002, Zita, TESC Review simple harmonic oscillators Examples and energy Damped harmonic motion Phase space.
Simple Pendulum A simple pendulum also exhibits periodic motion A simple pendulum consists of an object of mass m suspended by a light string or.
Associate Professor: C. H.L IAO. Contents:  3.1 Introduction 99  3.2 Simple Harmonic Oscillator 100  3.3 Harmonic Oscillations in Two Dimensions 104.
Vol. 3 Main Contents : 1.Vibration 2.Wave---Propagation of vibration or field. 3.Wave optics---Propagation of light Vibration and Wave Modern Physics 4.
Chapter 14 Outline Periodic Motion Oscillations Amplitude, period, frequency Simple harmonic motion Displacement, velocity, and acceleration Energy in.
Pendulums and Resonance
Copyright © 2010 Pearson Education, Inc. Lecture Outline Chapter 13 Physics, 4 th Edition James S. Walker.
Passive Acoustic Radiators Justin Yates, Wittenberg University Spring 2014.
Chapter 14 - Oscillations
1 Lecture D32 : Damped Free Vibration Spring-Dashpot-Mass System Spring Force k > 0 Dashpot c > 0 Newton’s Second Law (Define) Natural Frequency and Period.
11/11/2015Physics 201, UW-Madison1 Physics 201: Chapter 14 – Oscillations (cont’d)  General Physical Pendulum & Other Applications  Damped Oscillations.
SECOND ORDER LINEAR Des WITH CONSTANT COEFFICIENTS.
Chapter 1 - Vibrations Harmonic Motion/ Circular Motion Simple Harmonic Oscillators –Linear, Mass-Spring Systems –Initial Conditions Energy of Simple Harmonic.
Simple Harmonic Motion and Elasticity The Ideal Spring and Simple Harmonic Motion spring constant Units: N/m.
APPLIED MECHANICS Lecture 05 Slovak University of Technology
Advanced Engineering Mathematics by Erwin Kreyszig Copyright  2007 John Wiley & Sons, Inc. All rights reserved. Engineering Mathematics Lecture 05: 2.
Chapter 14 Oscillations
Fluid Dynamics How does conservation of mass apply in a fluid? How does conservation of energy apply in a fluid? What is laminar flow? What is turbulence.
Physics 321 Hour 11 Simple and Damped Harmonic Oscillators.
PH 421: Oscillations - do not distribute
Chapter 8 Vibration A. Free vibration  = 0 k m x
Oscillatory motion (chapter twelve)
Chapter 19 Physics A First Course Vibrations, Waves, and Sound.
1FCI. Prof. Nabila.M.Hassan Faculty of Computer and Information Basic Science department 2012/2013 2FCI.
Damped and Forced Oscillations
Damped Harmonic Motion  Simple harmonic motion in which the amplitude is steadily decreased due to the action of some non-conservative force(s), i.e.
Ball in a Bowl: F g F N F g F N  F  F Simple Harmonic Motion (SHM) Stable Equilibrium (restoring force, not constant force)
Main Menu Salas, Hille, Etgen Calculus: One and Several Variables Copyright 2003 © John Wiley & Sons, Inc. All rights reserved. Bernoulli Equations: Homogeneous.
Damped Free Oscillations
Damped harmonic oscillator
Chapter 8 Solving Second order differential equations numerically.
PHY238Y Lecture 3 Damped oscillations Forced oscillations. Resonance References: Halliday, Resnick, Walker: Fundamentals of Physics, 6 th edition, John.
-Damped and Forces Oscillations -Resonance AP Physics C Mrs. Coyle.
OSCILLATIONS spring pendulum.
Modeling with Higher-Order Differential Equations
Physics 8.03 Vibrations and Waves
Physics 3 – Aug 22, 2017 P3 Challenge –
Solving the Harmonic Oscillator
AP Physics Sections 11-4 to 11-6 Simple pendulum,
10.4 The Pendulum.
Physics 2 – May 1, 2018 P3 Challenge –
Physics 111 Practice Problem Solutions 14 Oscillations SJ 8th Ed
Physics A First Course Vibrations, Waves, and Sound Chapter 19.
Lecture Outline Chapter 13 Physics, 4th Edition James S. Walker
Lecture 22 Second order system natural response
Chapter 18: Elementary Differential Equations
1940 Tacoma Narrows Bridge Collapse
Physics 319 Classical Mechanics
Presentation transcript:

Will Bergman and Mike Ma Harmonic Oscillators Will Bergman and Mike Ma

Overview Simple Harmonic Motion Driven Simple Harmonic Oscillators Spring and Mass Periodic Driving Force General Form Resonance Damped Simple Harmonic Oscillators Tacoma Bridge Example Conclusion and Further Applications Underdamped Case Overdamped Case Critically Damped Case

Spring and Mass 𝐹=𝑚𝑎 𝑚 𝑑 2 𝑥 𝑑 𝑡 2 =−𝑘𝑥 Guess: 𝑥 𝑡 = 𝑒 𝑟𝑡 𝑚 𝑑 2 𝑥 𝑑 𝑡 2 =−𝑘𝑥 Guess: 𝑥 𝑡 = 𝑒 𝑟𝑡 𝑟 1 =+𝑖 𝑘 𝑚 , 𝑟 2 =−𝑖 𝑘 𝑚 𝑥 𝑡 = 𝐶 1 𝑥 1 𝑡 + 𝐶 2 𝑥 2 𝑡 𝑥 𝑡 = 𝐶 1 𝑒 𝑟 1 𝑡 + 𝐶 2 𝑒 𝑟 1 𝑡 (Taylor, 2003) https://commons.wikimedia.org/wiki/File:Simple_harmonic_oscillator.gif

General Form 𝑚 𝑑 2 𝑥 𝑑 𝑡 2 =−𝑘𝑥 𝑚 𝑑 2 𝑥 𝑑 𝑡 2 =−𝑘𝑥 𝑥 𝑡 = 𝐶 1 + 𝐶 2 𝑐𝑜𝑠 𝑤𝑡 +𝑖 𝐶 1 − 𝐶 2 𝑠𝑖𝑛 𝑤𝑡 𝑥 𝑡 =𝐵 1 𝑐𝑜𝑠 𝑤𝑡 + 𝐵 2 𝑠𝑖𝑛 𝑤𝑡 (Taylor, 2003)

Damped Simple Harmonic Oscillators B – damping constant 𝑤 0 - natural frequency Relationship between B and 𝑤 0 determine different cases of damping Solution form: 𝑥 𝑡 = 𝑒 𝑟𝑡

Underdamped Case (𝐵< 𝑤 0 ) 𝐵 2 − 𝑤 0 2 =𝑖 𝑤 0 2 − 𝐵 2 =𝑖 𝑤 1 𝑥 𝑡 =𝑒 −𝐵𝑡 ( 𝐶 1 𝑒 𝑖 𝑤 1 𝑡 + 𝐶 2 𝑒 −𝑖 𝑤 1 𝑡 ) Amplitude of oscillations decrease exponentially (Taylor, 2003)

Overdamped Case (𝐵> 𝑤 0 ) 𝑥 𝑡 = 𝑒 −𝐵𝑡 ( 𝐶 1 𝑒 𝐵 2 − 𝑤 0 2 𝑡 + 𝐶 2 𝑒 − 𝐵 2 − 𝑤 0 2 𝑡 ) No Oscillations! (Taylor, 2003)

Critically Damped Case (𝐵= 𝑤 0 ) Repeated Eigenvalues 𝐵= 𝑤 0 is a bifurcation value 𝑥 𝑡 = 𝑒 −𝐵𝑡 𝑥(𝑡)=𝑡𝑒 −𝐵𝑡 𝑥 𝑡 = 𝐶 1 𝑒 −𝐵𝑡 + 𝐶 2 𝑡𝑒 −𝐵𝑡 (Blanchard et al., 2012) (Taylor, 2003)

Driven Simple Harmonic Oscillators 𝑑 2 𝑥 𝑑 𝑡 2 +𝐵 𝑑𝑥 𝑑𝑡 + 𝑤 0 2 𝑥=𝑓(𝑡) Solution = general solution of homogeneous equation (unforced) + one particular solution to nonhomogeneous equation (forced) 𝑥 𝑡 = 𝐶 1 𝑥 1 𝑡 + 𝐶 2 𝑥 2 𝑡 + 𝑥 𝑝 (𝑡) Resonance- the frequency of the driving force is equal to the natural frequency of the oscillating system http://www.acs.psu.edu/drussell/Demos/SHO/mass-force.html

Conclusion and Further Applications of Theory https://www.youtube.com/watch?v=vPZuHFrawz4 https://www.youtube.com/watch?v=3mclp9QmCGs

References https://commons.wikimedia.org/wiki/File:Simple_harmonic_oscillator.gif Taylor, John R. "Chapter 5: Oscillations." Classical Mechanics. Sausalito, CA: U Science, 2005. 161-203. Print. Blanchard, Paul, Robert L. Devaney, and Glen R. Hall. "Chapter 2.3: The Damped Harmonic Oscillator." Differential Equations. Boston, MA: Brooks/Cole, Cengage Learning, 2012. 183-88. Print. http://www.acs.psu.edu/drussell/Demos/SHO/mass-force.html